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A block A of mass m1m_1 rests on a horizontal table. A light string connected to it passes over a frictionless pulley at the edge of the table and from its other end, another block B of mass m2m_2 is suspended. The coefficient of kinetic friction between block A and the table is μk\mu_k. When block A is sliding on the table, the tension in the string is:

A

(m2+μkm1)g(m1+m2)\frac{(m_2 + \mu_k m_1)g}{(m_1 + m_2)}

B

(m2μkm1)g(m1+m2)\frac{(m_2 - \mu_k m_1)g}{(m_1 + m_2)}

C

m1m2(1μk)g(m1+m2)\frac{m_1 m_2 (1 - \mu_k)g}{(m_1 + m_2)}

D

m1m2(1+μk)g(m1+m2)\frac{m_1 m_2 (1 + \mu_k)g}{(m_1 + m_2)}

Step-by-Step Solution

  1. System Analysis: Block B (m2m_2) moves vertically downwards and block A (m1m_1) moves horizontally. Both share the same magnitude of acceleration aa because they are connected by an inextensible string.
  2. Equations of Motion:
  • For Block B (m2m_2): The forces are weight m2gm_2g (down) and tension TT (up). Since it accelerates down: m2gT=m2a...(i)m_2g - T = m_2a \quad \text{...(i)}
  • For Block A (m1m_1): The forces are tension TT (forward) and kinetic friction fkf_k (backward). The vertical forces balance (N=m1gN = m_1g), so fk=μkN=μkm1gf_k = \mu_k N = \mu_k m_1g. Since it accelerates forward: Tfk=m1aTμkm1g=m1a...(ii)T - f_k = m_1a \Rightarrow T - \mu_k m_1g = m_1a \quad \text{...(ii)}
  1. Finding Acceleration: Add equations (i) and (ii) to eliminate TT: m2gμkm1g=(m1+m2)am_2g - \mu_k m_1g = (m_1 + m_2)a a=g(m2μkm1)m1+m2a = \frac{g(m_2 - \mu_k m_1)}{m_1 + m_2}
  2. Finding Tension: Substitute aa back into equation (ii): T=m1a+μkm1gT = m_1a + \mu_k m_1g T=m1[g(m2μkm1)m1+m2]+μkm1gT = m_1 \left[ \frac{g(m_2 - \mu_k m_1)}{m_1 + m_2} \right] + \mu_k m_1g T=m1m2gμkm12g+μkm12g+μkm1m2gm1+m2T = \frac{m_1 m_2 g - \mu_k m_1^2 g + \mu_k m_1^2 g + \mu_k m_1 m_2 g}{m_1 + m_2} T=m1m2g(1+μk)m1+m2T = \frac{m_1 m_2 g (1 + \mu_k)}{m_1 + m_2} (Reference: NCERT Class 11, Physics Part I, Chapter 5, Section 5.10 and Example 5.9).
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